The History of The
Principle of Self-Complementarity.
From the backgrounds of the origination and the discovery
to the extensions of the principle.
|
| (Minus number shows background). |
| －４ |
１９４１ |
| New expressions of the electromagnetic fields where both the electric and the magnetic quantities are treated on an equal basis. |
|
J. A. Stratton (U.
S. A.) |
|
| －３ |
１９４５ |
| A relationship between two radiation impedances for a narrow slot antenna and a complementary
wire antenna derived from a classical
antenna theory. |
| Z1Z2≒(Z0/2)2 |
T.
Matsumoto (Hokkaido Univ.)
M. Ito (Hiroshima Tech. Coll.)
(1946)
H. G. Booker (U. K.) |
|
| －２ |
１９４５ |
| Babinet's Principle in electromagnetic fields. |
| M. Kotani (Univ. of Tokyo), G. Sunouchi (Tohoku Univ.) |
|
| －１ |
１９４７ |
| A general relationship between two input impedances for an arbitrarily shaped slot
antenna and a complementary planar sheet antenna. |
| Z1Z2 =(Z0/2)2 |
Y. Mushiake (Tohoku Univ.) |
|
| 0 |
１９４８ |
|
| １ |
１９４８ |
|
Rotationally symmetric two-terminal self-complementary
planar antenna.
|
| Balanced type, 60π≒188.4 [Ω]. |
|
| Y. Mushiake (Tohoku Univ.) |
|
| ２ |
１９４８ |
|
Axially symmetric two-terminal self-complementary planar antenna.
|
| Unbalanced type, 60π≒188.4 [Ω]. |
| Y. Mushiake (Tohoku Univ.) |
|
| ３ |
１９５９ |
|
Rotationally
symmetric four-terminal self-complementary planar antenna (turnstile type)
|
Star-connection type, 30 π≒ 133.2 [Ω] each. |
| Y. Mushiake (Tohoku Univ.) |
|
| ４ |
１９５９ |
|
Rotationally
symmetric multi-terminal self-complementary planar antennas.
|
|
Star-,
ring-, and other connections for various values of input impedances.
|
| G. A. Deschamps (U. S. A.) |
|
| ５ |
１９６３ |
|
Three-dimensional multi(N)-planar axially symmetric two-terminal self-complementary
antenna.
|
| Unbalanced type, 60π/ N ≒ 94.2 [Ω], for N=2. |
| Y. Mushiake (Tohoku Univ.) |
|
| ６ |
１９７２ |
|
Checkerboard type multi-terminal
self-complementary planar antenna.*
|
| Balanced type, 60π≒ 188.4 [Ω] each.. |
| N. Inagaki (Nagoya Tech. Univ.) |
|
| ７ |
１９７８ |
|
Modified
three-dimensional self-complementary antenna.* *
|
| Unbalanced type, 30π≒ 133.2 [Ω]. |
| T. Kasahara, T. Ishizone, Y. Mushiake (Tohoku Univ.) |
|
| ８ |
１９８１ |
|
Modified
three-dimensional self-complementary transmission line.
|
| Unbalanced type, 30π≒ 133.2 [Ω]. |
| T. Ishizone (Tohoku Univ.) |
|
| ９ |
１９８２ |
| Co-planar stacked self-complementary antenna. |
| Unbalanced type, 60π≒ 188.4 [Ω] each. |
| Y. Mushiake (Tohoku Univ.) |
|
| １０ |
１９８２ |
| Side-by-side stacked self-complementary antenna. |
| Unbalanced type, 60π≒ 188.4 [Ω] each. |
| Y. Mushiake (Tohoku Univ.) |
|
| １１ |
１９８２ |
| Compound-stacked self-complementary antenna. |
| Unbalanced type, 60π≒ 188.4 [Ω] each. |
| Y. Mushiake (Tohoku Univ.) |
|
| １２ |
１９９４ |
|
Axially
symmetric self-complementary antenna with loaded multi-element.
|
| Unbalanced type, 60π≒ 188.4 [Ω] each. |
| Y. Mushiake (Tohoku Univ.) |
|
|
|
|
|
* Freedom in the shape
is restricted to similitude-transformation.
* * Theoretical proof for general cases has not been
succeeded, except for the monopoly-slot type array antenna.
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of the